Course: PHY 6346, Electromagnetic Theory 1,
Meeting times: MWF, Period 8 (3:00-3:50pm), room 1101
Instructor: J. N. Fry, Office: 2172,
Phone: 392-6692, e-mail:
fryatphys.ufl.edu,
Office Hours: M 9, Tu/Th 6
[schedule]
Graders: Xiao Chen, Office: B51,
Phone: 392-0477,
e-mail:
xiaochenatphys.ufl.edu, Office Hour: W 5
Luyi Yan, Office: 1133,
Phone: 273-4643,
e-mail:
yan88130atphys.ufl.edu, Office Hour: W 5
Course Description: PHY 6346 is the first semester of the graduate core sequence in Electromagnetism, studying Maxwell's equations in general and in specific situations. The objectives of the course are (i) to study electrodynamics at a theoretically sophisticated level; (ii) to develop mathematical techniques useful for solving problems in E&M as well as other areas of physics; (iii) to develop problem solving skills; (iv) to prepare the student (if necessary) for the preliminary exam. Topics to be covered include
Grading: Grading will be based 50% on periodic homework sets, and 25% each on a midterm and final exam. The midterm exam will be on or about Thursday, October 15, 8:00–10:00 pm (7:30?), in room NEB 202. [solution] [distribution]. The final exam is Thursday, December 17, 5:30–7:30pm (Exam Group 17E). some sample problems [solution] [distribution] [average = 56 ± 11, median = 55, quartiles = 49, 63]. Students are expected to complete work at the time it is due, or as soon as possible in case of illness or other accepted, documented unusual circumstance. Homework solutions will be posted as soon as all papers are turned in, and it is not fair to your colleagues to delay this. In extreme cases I will post the names of people who are holding up the availability of solutions. There will be no last-minute makeups accepted.
The following paragraphs of advice on how to do well in Physics
are lifted from one of my colleagues.
This is a graduate course, and you are free to make your own
choices, but you should think about what they say:
I do not plan to take daily attendance, but it is to your
advantage to attend class.
You may spend most of your time sleeping or texting, but in between you
will have the opportunity to learn what subjects I think are important,
and you can then concentrate on these subjects during your reading.
If by some unfortunate set of circumstances you do miss class, do not ask
me if I said anything important — everything that I say is important.
Instead, ask a classmate; she or he is likely to give an honest answer,
and you won't offend me.
There will be a substantial number of examples discussed in class
that are not in the textbook, and examples in class often appear on tests.
If you miss class you will not do well in this course.
Do the assigned homework.
This is the drudge part of physics, but it is absolutely necessary.
We will learn grand ideas and see their wondrous applications in class.
But, your understanding is only superficial unless you can apply these same
grand ideas to completely new circumstances.
In course work, this is usually done with homework problems.
Do not be surprised if the homework is frustrating at times;
solving one challenging problem makes the next much easier.
And homework problems often appear on tests.
Doing all of the homework is the easiest way to improve your grade.
Not doing homework is the easiest way to lower your grade.
homework-exam correlation and another
Required text:
Other books:
^{[1]} Gaussian units; ^{[2]} Lorentz units
Kevin Schmidt's Possibly Useful Books for Classical Electromagnetism, with comments
The following quote (attributed to Sidney Coleman) captures a common reaction to Jackson: Scientists tend to overcompress, to make their arguments difficult to follow by leaving out too many steps. They do this because they have a hard time writing and they would like to get it over with as soon as possible.... Six weeks of work are subsumed into the word “obviously.”
This and that:
Physical Constants from the
Particle Data Group
JavaScript Calculator with built-in SI and cgs constants [1996 values]
Math trivia,
Akira Hirose Math Notes
Charles Augustin de Coulomb,
Accuracy of Coulomb's law,
John Robison
More than you wanted to know about
δ-functions from
random vector field,
longitudinal vector field,
transverse vector field
Renormalized potential for an infinite line charge.
See also
arXiv:physics/0503107 (in Portuguese)
George Green, Mathematician (Nottinghamshire History),
George Green, Mathematician and Physicist
(The Mathematical Gazette),
The Green of Green Functions (Physics Today, December 2003),
From Darkness to Green
An Essay on the
Application of Mathematical
Analysis to the Theories of Electricity and Magnetism (1828)
[arXiv]
[google books]
Proof that the Neumann Green's function in electrostatics
can be symmetrized:
K. J. Kim and J. D. Jackson, Am. J. Phys. 61, 1144 (1993)
images in parallel mirrors
(closeup)
(image)
(image)
Potential at the center of a cube, 2d frame
Fourier sin series for step function
animation (135)
animation (pbs)
Fourier sin series for
δ(x−x')
(max = 8, 32,
128, 1024),
zoom
Green's function for 2d square
Harmonic functions
Legendre polynomials:
Rodrigues' Formula and recursions
Pl(cosθ)
vs. θ and
vs. (l+½)θ
Legendre polynomial expansion of step function
Spherical Harmonic Angular Distributions
Spherical Harmonics
Bessel functions,
P_{100}(cosθ),
zeroes
x_{0n},
x_{1n} of
J_{0}(x),
J_{1}(x)
Lecture −6 by Dr P B Agarwal (IIT Roorkee)
Bessel series expansion of step function
More about Bessel functions
NASA GSFC and NIMA Joint Geopotential Model,
NGA/NASA Earth Gravitational Model,
multipole amplitudes
André Marie Ampère
Magnetic Monopoles Song
Magnetic Monopole Searches
Evidence for Detection of a
Moving Magnetic Monopole,
B. Price, E. Shirk, W. Osborne, L. Pinsky,
Phys Rev Lett 35, 487 (1975) /
Further measurements and reassment
Phys Rev Lett D18, 1382 (1978).
First Results from a Superconductive Detector for
Moving Magnetic Monopoles, B. Cabrera,
Phys Rev Lett 48, 1378 (1982).
Elliptic integrals
Non-dipolar order
Magnetic shielding,
wikipedia,
MμMetal,
lessEMF
cylindrical bar magnet
Michael Faraday,
Joseph
Henry
Magnetic field diffusion (in)
[log t/τ = −5, 5, 1],
(out),
skin depth,
ELF submarine communication
Who was James Clerk Maxwell?,
A Dynamical Theory of the Electromagnetic Field,
J. Clerk Maxwell,
Phil. Trans. R. Soc. Lond. 155, 459 (1865).
John Henry Poynting,
radiation pressure,
A COMPARISON of the
FLUCTUATIONS in the PRICE
of WHEAT and in the
COTTON and SILK
IMPORTS into GREATK
BRITAIN,
Journal of the Royal Statistical Society 47,
33–64 (1884)
Cosmic Variance,
@dalcantonJD,
@RisaWechsler,
sean carroll,
@seanmcarroll,
Leaves on the Line,
@defjaf,
Cosmic Yarns,
@ktfreese,
In the Dark,
@telescoper,
@lbaudis,
Quantum Frontiers,
@preskill,
@LKrauss1,
@FrankWilczek,
The Insoluble Pancake,
Starts With a Bang!,
@StartsWithABang!
Skeetobite Weather,
SFWMD computer tracks,
HWRF
Lego LHC,
Collider,
Mr Higgs Twist,
[Les Horribles Cernettes]
LHC Street View
Bohemian Gravity,
I Will Derive
Let it Snow
Let it Snow
(Dean Martin),
High Tide Ventures Christmas,
The Twelve Days of Christmas
Homework: Problem solving is a skill learned only through practice. Take advantage of the homework as an opportunity to learn how to recognize the right approach to a problem before exam time and it becomes too late. While I encourage you to discuss the assignments with each other, what you turn in must represent your own work. As we also do when publishing research articles: if you obtain significant information from a published or human source, cite that source. This will often be as little as "Jackson, eq. (10.43)". If you work together, please identify other members of your working group. This edition of the textbook uses SI (mks) units, at least until the chapters on relativity. Correct solutions to the assigned problems will be in appropriate units. Best answers are reduced to simplest terms; ½ tan^{−1}[2az/(a^{2}−z^{2})] is and is not the same as tan^{−1}(z/a) . And, please be sure that in the end your elegant solution in fact answers the question asked! Three Tips for Solving Physics Problems / How to Solve Physics Problems
University Policies:
Students are expected to know and comply with
the University's policies regarding academic honesty
and use of copyrighted materials.
Cheating, plagiarism, or other violations of the Academic Honesty Guidelines
will not be tolerated and will be pursued through the University's
adjudication procedures.
“Students requesting classroom accommodations
must first register with the Disabilities Resources Program, located in
the Dean of Students Office, P202 Peabody Hall.
The Disabilities Resources Program will provide documentation to
the student, who must then deliver this documentation to the instructor
when requesting accommodations.”